Publisher's Note: This paper, originally published on 8 June 2023, was replaced with a corrected/revised version on 3 October 2023. If you downloaded the original PDF but are unable to access the revision, please contact SPIE Digital Library Customer Service for assistance.
We report on the time-resolved observation of transient laser-induced breakdown (LIB) during the leading edge of high-intensity petawatt-class laser pulses with peak intensities up to 6x10^21 W/cm^2 in interaction with dielectric cryogenic hydrogen jet targets. The results show that LIB occurs much earlier than what is typically expected following the concept of barrier suppression ionization and that the laser pulse duration dependence of LIB and laser-induced damage threshold (LIDT) is very relevant to high-intensity laser-solid interactions. We demonstrate an effective approach to determine the onset of LIB, i.e. the starting point of target pre-expansion, by comparing a laser contrast measurement with a characterization study of the target specific LIB thresholds.
The new short focal length experimental beamline at the BELLA PW, called iP2, was commissioned up to 17 J laser pulse energy, corresponding to a peak intensity of 1.2 × 1021 W/cm2 on target, based on a measured focal spot size with FWHM 2.7 μm and Gaussian equivalent pulse length of 40 fs. The ion acceleration performance was measured under variation of the laser pulse energy and length, and the laser spot size on target. A maximum proton energy of ∼ 40 MeV was observed in the target normal sheath acceleration regime using 13 μm thick Kapton foil targets. Surveys outside the radiation shielded accelerator cave showed very low radiation levels and there was no measurable activation of experimental installations after performing several tens of shots on target. Back reflections of the laser pulse from the target interaction were monitored and partially mitigated, but ultimately caused damage in the laser frontend. This prohibited further increase of the laser pulse energy beyond 17 J. Implementation of a double plasma mirror is expected to sufficiently suppress back reflections to allow for iP2 experiments at the full BELLA PW pulse energy.
We established an experimental platform for the investigation of the radiobiological effects of stable few-MeV laser-accelerated ions at the BELLA Center using a peak laser pulse intensity of 2x1019 W cm-2 [1]. The focal spot size of laser pulses from the BELLA PW laser system is large compared to that found in typical laser-driven ion beamlines, which resulted in reduced divergence and increased ion numbers [2]. Such beams are ideally suited for subsequent capture and transport with an active plasma lens (APL) [3]. Combined with our high shot rate capability (0.2 Hz), around 1000 shots at ultra-high instantaneous dose rates (0.6 Gy/shot resulting in 107 Gy/s), with a uniform dose distribution over a 1 cm diameter lateral area, could thus be delivered to biological cell sample cups, located in air at 1.7 m distance from the laser-target interaction. The proton beamline was complemented by online (integrating current transformer and scintillator) and offline (radiochromic films) beam diagnostics for dosimetry. This assembly was used to investigate the differential sparing of healthy tissues versus the tumor response under reduced oxygen conditions. This talk gives details on the proton beamline, dosimetry as well as preliminary cell irradiation results.
This work is supported by U.S. Department of Energy Office of Science, Offices of High Energy Physics and Fusion Energy Sciences, Contract No. DE-AC02-05CH11231 and LBNL Laboratory Directed Research and Development Grant, PI A. M. Snijders
[1] K. Nakamura, et al., Diagnostics, Control and Performance Parameters for the BELLA High Repetition Rate Petawatt Class Laser, IEEE J. Quantum Electron., 53, (2017), 1200121 [2] S. Steinke, et al., Acceleration of high charge ion beams with achromatic divergence by petawatt laser pulses, Phys. Rev. Accel. Beams, 23, (2020), 021302
[3] J. Van Tilborg, et al., Active Plasma Lensing for Relativistic Laser-Plasma-Accelerated Electron Beams, Phys. Rev. Lett., 115, (2015), 184802
KEYWORDS: Hydrogen, Laser beam diagnostics, Laser systems engineering, Plasma, Cryogenics, Ion beams, Computer simulations, Data conversion, Data analysis, Mode locking
The development of high-intensity short-pulse lasers in the Petawatt regime offers the possibility to design new compact accelerator schemes by utilizing high-density targets for the generation of ion beams with multiple 10 MeV energy per nucleon. The optimization of the acceleration process demands comprehensive exploration of the plasma dynamics involved, for example via spatially and temporally resolved optical probing. Experimental results can then be compared to numerical particle-in-cell simulations, which is particularly sensible in the case of cryogenic hydrogen jet targets [1]. However, strong plasma self-emission and conversion of the plasma’s drive laser wavelength into its harmonics often masks the interaction region and interferes with the data analysis. Recently, the development of a stand-alone and synchronized probe laser system for off-harmonic probing at the DRACO laser operated at the Helmholtz-Zentrum Dresden–Rossendorf showed promising performance [2].
Here, we present an updated stand-alone probe laser system applying a compact CPA system based on a synchronized fs mode-locked oscillator operating at 1030 nm, far off the plasma’s drive laser wavelength of 800 nm. A chirped volume Bragg grating (Optigrate Corp) is used as a hybrid stretcher and compressor unit. The system delivers 160 fs pulses with a maximum energy of 0.9 mJ. By deploying the upgraded probe laser system in the laser-proton acceleration experiment with the renewable cryogenic hydrogen jet target, the plasma self-emission could be significantly suppressed while studying the temporal evolution of the expanding plasma jet. Recorded probe images resemble those of z-pinch experiments with metal wires and indicate a sausage-like instability along the jet axis, which will be discussed.
References
[1] L. Obst, et al. Efficient laser-driven proton acceleration from cylindrical and planar cryogenic hydrogen jets. Sci. Rep., 7:10248, 2017.
[2] T. Ziegler, et al. Optical probing of high intensity laser interaction with micron-sized
cryogenic hydrogen jets. Plasma Phys. Control. Fusion, 2018. doi:10.1088/1361-6587/
aabf4f.
[3] C.P. João, et al. Dispersion compensation by two-stage stretching in a sub-400 fs, 1.2 mJ
Yb:CaF2 amplifier. Opt. Express, 22:10097–10104, 2014.
Extreme field gradients intrinsic to relativistic laser plasma interactions enable compact MeV proton accelerators with unique bunch characteristics. Yet, direct control of the proton beam profile is usually not possible. So far, only complex micro-engineering of the relativistic plasma accelerator itself and limited adoption of conventional beam optics provided access to global beam parameters that define propagation.
We present a novel, counter-intuitive all-optical approach to imprint detailed spatial information from the driving laser pulse to the proton bunch.
The concept was motivated by an effect initially observed in an experiment dedicated to laser-driven proton acceleration from a renewable micrometer sized cryogenic Hydrogen jet target at the 150 TW Draco laser at HZDR. A compact, recollimating single plasma mirror was used to enhance the temporal laser contrast, which could be monitored on a single-shot base by means of self-referenced spectral interferometry with extended time excursion (SRSI-ETE) at unprecedented dynamic and temporal range. Unexpectedly, the accelerated proton beam profile showed in this experiment prominent features of the collimated laser beam, such as the shadow of obstacles inserted deliberately in the beam.
In a series of further experiments, the spatial profile of the energetic proton bunch was found to exhibit identical features as the fraction of the laser pulse passing around a target of limited size. The formation of quasi-static electric fields in the beam path by ionization of residual gas in the experimental chamber results in asynchronous information transfer between the laser pulse and the naturally delayed proton bunch.
Such information transfer between the laser pulse and the naturally delayed proton bunch is attributed to the formation of quasi-static electric fields in the beam path by ionization of residual gas. Essentially acting as a programmable memory, these fields provide access to a new level of proton beam manipulation.
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print or electronic format on
SPIE.org.
INSTITUTIONAL Select your institution to access the SPIE Digital Library.
PERSONAL Sign in with your SPIE account to access your personal subscriptions or to use specific features such as save to my library, sign up for alerts, save searches, etc.